Application of the First Order ODE Electric Circuits - RC
\(L\frac{di}{dt}+Ri=E(t)\) \(0.1\frac{di}{dt}+(15)i=30\) \(\frac{di}{dt}+150i=300\) \(p(t)=150~~~,~~~q(t)=300\) \(u(t)=e^{\int_{}{}150dt}\) \(u(t)=e^{150t}\) \(\frac{d}{dt}(e^{150t}i)=e^{150t}(300)\) \(i=\frac{1}{e^{150t}}(\int_{}{}e^{150t}300dt)\) \(i=\frac{1}{e^{150t}}(2e^{150t}+c)\) \(i=2+\frac{C}{e^{150t}}\) when \(i=0,t=0\) \(0=2+c\) \(c=-2\) \(i=2-\frac{2}{e^{150t}}\) when \(t~\rightarrow~\infty\) \(i=2-\frac{2}{\infty}\) \(i=2\)
Is my working correct?
\(L\frac{di}{dt}+Ri=E(t)\) \(20\frac{di}{dt}+2i=120\) \(\frac{di}{dt}+\frac{1}{10}i=6\) \(p(t)=\frac{1}{10}~~~,~~~q(t)=6\) \(u(t)=e^{\int_{}{}\frac{1}{10}dt}\) \(u(t)=e^{\frac{1}{10}t}\) \(\frac{d}{dt}(e^{\frac{1}{10}t}i)=e^{\frac{1}{10}t}(6)\) \(i=\frac{1}{e^{\frac{1}{10}t}}(\int_{}{}e^{\frac{1}{10}t}(6)dt)\) \(i=\frac{1}{e^{\frac{1}{10}t}}(60e^{\frac{t}{10}}+c)\) \(i=60+\frac{C}{e^{\frac{t}{10}}}\) when \(i=0,t=0\) \(0=60+C\) \(C=-60\) \(i=60-\frac{60}{e^{\frac{t}{10}}}\)
Is this one correct too?
@nuts is our resident electrical engineering major
\(\color{#0cbb34}{\text{Originally Posted by}}\) @Shadow @nuts is our resident electrical engineering major \(\color{#0cbb34}{\text{End of Quote}}\) >.< he might be busy at this hour
Well he is your best shot so might as well tag him (:
seems legit enough
\(\color{#0cbb34}{\text{Originally Posted by}}\) @Shadow Well he is your best shot so might as well tag him (: \(\color{#0cbb34}{\text{End of Quote}}\) haha,alright XD
t->infinity current is correct
i can look in more detail if you want... might be too lazy to actually go through the math so i'll just run on simulator lol
just wanna make sure whether the answer was right hmm,what kind of simulator do u use? :o
in this case, I can't let \(C=\frac{C}{e^{150t}}\) right?
nvm i didnt' realize you posted 2 problems. the first one looks ok... the second one is basically a repeat of the first so it's not worth checking lol
\(\color{#0cbb34}{\text{Originally Posted by}}\) @nuts nvm i didnt' realize you posted 2 problems. the first one looks ok... the second one is basically a repeat of the first so it's not worth checking lol \(\color{#0cbb34}{\text{End of Quote}}\) yeah,if first one was right, Im pretty the second should be right XD
honestly the closed form solution of RL, RC, and RLC circuits are readily available online... I usually just look them up on electronicsws or on wikipedia
pretty sure**
of course in an ODE class it's more important to derive time domain solutions from first principles (KVL, KCL, and doing the math), but in practice we typically take things to the frequency domain or the s-domain (fourier/laplace transforms respectively) and quickly find the solution
but yeah your answers seem to match reasonable numbers
\(\color{#0cbb34}{\text{Originally Posted by}}\) @nuts of course in an ODE class it's more important to derive time domain solutions from first principles (KVL, KCL, and doing the math), but in practice we typically take things to the frequency domain or the s-domain (fourier/laplace transforms respectively) and quickly find the solution \(\color{#0cbb34}{\text{End of Quote}}\) Thanks for the tip
later you might learn laplace transforms, and you will see how they make solving linear odes a trivial task...
\(\color{#0cbb34}{\text{Originally Posted by}}\) @nuts but yeah your answers seem to match reasonable numbers \(\color{#0cbb34}{\text{End of Quote}}\) yay! Thanks bro! LOL,just finish chapter 1 >.< Omg,still got 4 more chapters left.
\(\color{#0cbb34}{\text{Originally Posted by}}\) @nuts later you might learn laplace transforms, and you will see how they make solving linear odes a trivial task... \(\color{#0cbb34}{\text{End of Quote}}\) owh I c,that's interesting :D
yeah basically if you think about it the solution to any ODE comes in the form \(\Huge e^{(\sigma+i\omega)x}\) (either a real exponential or a complex exponential which is a real exponential multiplied by a sinusoid). Recognizing that the derivative of this expression and the integral of this expression are just constant factors, the laplace transform takes differential equations into an s-domain world where everything is thought of in terms of these exponentials making it easier to perform calculus on differential equations (turns calculus into algebra). You then take the inverse laplace transform to get your answer. Of course you have to worry about convergence and the inverse laplace transform can often be a pain, but with laplace transform tables it's often times faster.
**linear ODE
woah,can't wait to read that chapter,hehe Thanks for the info also,thanks for the help ^
yup np
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